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From all-metal aromatic clusters to
 open-shell spherical aromaticity

                   Jordi Poater
       Institut de QuímicaComputacional
         and Departament de Química,
              Universitat de Girona
Fullerenes
                                               1985

• The concept of
  aromaticityis no             Nanotubes       1991

  longer confined to
  "carbon chemistry"
  but can be applied                           2001   All-metal Aromaticity
  to the entire
  periodic table.      d-orbital Aromaticity
                                               2005


                                               2007 -Aromaticity


                       f-orbital Aromaticity   2008
Open-shellsphericalaromaticity
• Hückel’s 4n+2 rule
                                              coronene                  pyrene


                                           Dnh


                                              n




  Aromaticityof (4n+2)p-annuleneswithDnhsymmetry comes fromthefulfillmentof a
  closed-shellthatprovides extra stability.
Open-shellsphericalaromaticity
• Baird’s 4n rule


                                         Dnh



                                               n



  Aromaticityoflowest-lyingtripletstateof(4n)p-annuleneswithDnhsymmetry comes
  fromthesame-spinhalf-filleddegeneratehighest-occupiedMOsthatprovides extra
  stability.
Open-shellsphericalaromaticity
• Hirsch’s 2(n+1)2ruleforsphericalaromaticity
                     Rotor rigid solution


 n=3                                                                              32

 n=2                                                                              18

 n=1                                                                              8

 n=0                                                                              2

               2, 8, 18, 32, 50, 72, 98… = 2(n+1)2
           A. Hirsch, Z. Chen and H. Jiao, Angew. Chem. Int. Ed. 2000, 39, 3915
Open-shellsphericalaromaticity
             • Hirsch’s
               2(n+1)2ruleforsphericalaromatici
               ty




                Z. Cheng and R. B. Bruce Chem. Rev.,2005, 105, 3613
Open-shellsphericalaromaticity
                    PLANAR             SPHERICAL

CLOSED-SHELL    4n+2 Hückel’s rule     2(n+1)2 Hirsch’s rule




               4n lowest-lying
OPEN-SHELL     triplet excited state           ?
               Baird’s rule
Open-shellsphericalaromaticity
• 2n2+2n+1 (S=n+1/2) rulefor open-shellsphericalaromaticity



 n=3                                                                32
 n=2                                                                18
 n=1                                                                8
 n=0                                                                2

            1, 5, 13, 25, 41, 61, 75… = 2n2+2n+1; (S=n+1/2)

              J. Poater and M. Solà Chem. Commun. 2011, 47, 11647
Open-shellsphericalaromaticity
  • Aromaticityindices


Magnetic shielding tensor

                          Multicenter delocalization indices
                              A = {A1, A2, …, AN}
 For monodeterminantal WFs:                      I ring ( A )       n           i1    niN S i1i2 A1 S i2i3 A2  S iN i1 AN 
                                                                  i1 ,i2 ,,i N

 M. Giambiagi, M. S. de Giambiagi, C. D. dos Santos Silva and A. P. de Figuereido,Phys. Chem. Chem. Phys. 2000, 2, 3381

                                                 1
                                    MCI ( A ) 
                                                2N
                                                              I
                                                             P( A )
                                                                           ring        ( A)
                        P. Bultinck, R. Ponec and S. van Damme,J. Phys. Org. Chem. 2005, 18, 706
Open-shellsphericalaromaticity


         Systems symm.         NICS(1)zz      MCI          r(C,C)    Spin
           C202+       Ih         -7.4        0.020        1.447     S=0
           C207+       Ih         -4.0        0.035        1.494    S = 3/2
           C205-       Ih         -18.0       0.024        1.508    S = 7/2




     J. Poater and M. Solà Chem. Commun. 2011, 47, 11647
Open-shellsphericalaromaticity
      Systems symm          Ring    NICS(1)zz    MCI       BLA    Spin
         C60        Ih     6-MR        0.8      0.018 0.058       S=0
                           5-MR       21.5      0.011
        C601-       Ih     6-MR        -1.4     0.017 0.002 S = 11/2
                           5-MR       -19.9     0.049
        C6019+      Ih     6-MR       -14.9     0.019 0.013      S = 9/2
                           5-MR       -25.3     0.041
        C6010+      Ih     6-MR       -18.6     0.011 0.030       S=0
                           5-MR       -29.5     0.017

     J. Poater and M. Solà Chem. Commun. 2011, 47, 11647
Open-shellsphericalaromaticity
    Systems    symm.      Ring     NICS(1)zz      MCI       BLA      Spin

      C80         S6      5-MR        10.7       0.019               S=0
                          6-MR        -5.2       0.012      0.025
                          5-MR        26.3       0.018
                          6-MR        11.3       0.014      0.001
                          6-MR        -5.1       0.012      0.025
     C808+        Ih      6-MR        -7.2       0.011      0.015    S=0
                          5-MR        -4.0       0.017
     C805-        Ih      6-MR       -20.8       0.019      0.012   S = 13/2
                          5-MR        -5.5       0.034
      J. Poater and M. Solà Chem. Commun. 2011, 47, 11647
Open-shellsphericalaromaticity




    Systems   symm.   NICS(1)zz   MCI      Spin
    Ge122-     Ih        -5.5     0.049    S=0
    Ge121-     Ih      -405.9     0.113   S = 5/2
    Ge124+     Ih       -69.0     0.088    S=0
All-metal aromatic clusters
• All-metal and semimetal aromatic clusters
  are among the most exciting molecules
  synthesized since the beginning of the present
  century.
• These compounds can have not only the
  conventional p-(anti)aromaticity of classical
  organic compounds, but also - or even - and
  -(anti)aromaticity, thus giving rise to the so-
  called multifold aromaticity.
All-metal aromatic clusters
• Thetendencyofp-electrons in
  classicalorganicaromaticmoleculesisalwaystolocalizethedoublebond
  s (distortivecharacter), againstthedelocalizingforceofthe-electrons.




        S.C.A.H. Pierrefixe, F.M. Bickelhaupt, Chem. Eur. J. 2007, 13, 6321
• Thus, whilemany of thepropertiesattributedtoaromaticity derive
  fromthep-electrons, the-electrons are
  theonesresponsibleforthesymmetricframework of
  monocyclicaromaticcompounds.
All-metal aromatic clusters
• Al42-wasthefirstall-metal compoundssynthesized, containinga pair of
  delocalized p-electrons (orbital 1a2u) and two pairs of -electrons (orbitals
  1b2g and 2a1g) that contribute to the overall aromaticity of this species.
  X. Li, A.E. Kuznetsov, H.F. Zhang, A.I. Boldyrev, L.S. Wang, Science 2001, 291, 859.




• Thus, Al42- can be considered as a “3-
  fold” aromatic system ( + paromatic)
All-metal aromatic clusters
• Are the p-electrons of the Al42- cluster
  distortive, i.e., do they work against the
  regular "aromatic" structure with
  delocalized, equivalent bonds? Or is this
  propensity a characteristic of only classical
  aromatic organic molecules?



    J. Poater, F. Feixas, F.M. Bickelhaupt and M. Solà Chem. Commun. 2011, 47, 11647
All-metal aromatic clusters
• AmsterdamDensityFunctional
• BP86/TZ2P, QUILD
• EnergyDecompositionAnalysis
    ∆E : M2- (aaa) + M2- (bbb) M42-
    ∆E =∆Eprep + ∆Eint
    ∆Eint = ∆Velstat + ∆EPauli + ∆Eoi
    ∆Eoi = SG ∆EG
    ∆Eint = ∆Velstat + “total ” + “total p”
   J. Poater, F. Feixas, F.M. Bickelhaupt and M. Solà Chem. Commun. 2011, 47, 11647
All-metal aromatic
     clusters




  J. Poater, F. Feixas, F.M. Bickelhaupt and M. Solà Chem. Commun. 2011, 47, 11647
All-metal aromatic
                clusters

50

40

30                                                    total 

20
                                                      DEint
10

 0
                                                      total p
      90       92      94       96      98      100
-10
                                                      DVelstat
-20

-30




           •Equivalenttrendstothosefound in
           benzene.
                J. Poater, F. Feixas, F.M. Bickelhaupt and M. Solà Chem. Commun. 2011, 47, 11647
NICS(1b2g)= +10.8ppm
NICS(2a1g)=-3.9ppm
ACKNOWLEDGMENTS




Prof. Dr. MiquelSolà(UdG)                   Prof. Dr. F. Matthias Bickelhaupt
               Dr. FerranFeixas (San Diego, USA)
http://iqc.udg.edu


19/4/2012 Toulouse     RECENT ADVANCES IN AROMATICITY   27

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XXVIII Reunió Anual XRQTC

  • 1.
  • 2. From all-metal aromatic clusters to open-shell spherical aromaticity Jordi Poater Institut de QuímicaComputacional and Departament de Química, Universitat de Girona
  • 3. Fullerenes 1985 • The concept of aromaticityis no Nanotubes 1991 longer confined to "carbon chemistry" but can be applied 2001 All-metal Aromaticity to the entire periodic table. d-orbital Aromaticity 2005 2007 -Aromaticity f-orbital Aromaticity 2008
  • 4. Open-shellsphericalaromaticity • Hückel’s 4n+2 rule coronene pyrene Dnh n Aromaticityof (4n+2)p-annuleneswithDnhsymmetry comes fromthefulfillmentof a closed-shellthatprovides extra stability.
  • 5. Open-shellsphericalaromaticity • Baird’s 4n rule Dnh n Aromaticityoflowest-lyingtripletstateof(4n)p-annuleneswithDnhsymmetry comes fromthesame-spinhalf-filleddegeneratehighest-occupiedMOsthatprovides extra stability.
  • 6. Open-shellsphericalaromaticity • Hirsch’s 2(n+1)2ruleforsphericalaromaticity Rotor rigid solution n=3 32 n=2 18 n=1 8 n=0 2 2, 8, 18, 32, 50, 72, 98… = 2(n+1)2 A. Hirsch, Z. Chen and H. Jiao, Angew. Chem. Int. Ed. 2000, 39, 3915
  • 7. Open-shellsphericalaromaticity • Hirsch’s 2(n+1)2ruleforsphericalaromatici ty Z. Cheng and R. B. Bruce Chem. Rev.,2005, 105, 3613
  • 8. Open-shellsphericalaromaticity PLANAR SPHERICAL CLOSED-SHELL 4n+2 Hückel’s rule 2(n+1)2 Hirsch’s rule 4n lowest-lying OPEN-SHELL triplet excited state ? Baird’s rule
  • 9. Open-shellsphericalaromaticity • 2n2+2n+1 (S=n+1/2) rulefor open-shellsphericalaromaticity n=3 32 n=2 18 n=1 8 n=0 2 1, 5, 13, 25, 41, 61, 75… = 2n2+2n+1; (S=n+1/2) J. Poater and M. Solà Chem. Commun. 2011, 47, 11647
  • 10. Open-shellsphericalaromaticity • Aromaticityindices Magnetic shielding tensor Multicenter delocalization indices A = {A1, A2, …, AN} For monodeterminantal WFs: I ring ( A )  n i1  niN S i1i2 A1 S i2i3 A2  S iN i1 AN  i1 ,i2 ,,i N M. Giambiagi, M. S. de Giambiagi, C. D. dos Santos Silva and A. P. de Figuereido,Phys. Chem. Chem. Phys. 2000, 2, 3381 1 MCI ( A )  2N I P( A ) ring ( A) P. Bultinck, R. Ponec and S. van Damme,J. Phys. Org. Chem. 2005, 18, 706
  • 11. Open-shellsphericalaromaticity Systems symm. NICS(1)zz MCI r(C,C) Spin C202+ Ih -7.4 0.020 1.447 S=0 C207+ Ih -4.0 0.035 1.494 S = 3/2 C205- Ih -18.0 0.024 1.508 S = 7/2 J. Poater and M. Solà Chem. Commun. 2011, 47, 11647
  • 12. Open-shellsphericalaromaticity Systems symm Ring NICS(1)zz MCI BLA Spin C60 Ih 6-MR 0.8 0.018 0.058 S=0 5-MR 21.5 0.011 C601- Ih 6-MR -1.4 0.017 0.002 S = 11/2 5-MR -19.9 0.049 C6019+ Ih 6-MR -14.9 0.019 0.013 S = 9/2 5-MR -25.3 0.041 C6010+ Ih 6-MR -18.6 0.011 0.030 S=0 5-MR -29.5 0.017 J. Poater and M. Solà Chem. Commun. 2011, 47, 11647
  • 13. Open-shellsphericalaromaticity Systems symm. Ring NICS(1)zz MCI BLA Spin C80 S6 5-MR 10.7 0.019 S=0 6-MR -5.2 0.012 0.025 5-MR 26.3 0.018 6-MR 11.3 0.014 0.001 6-MR -5.1 0.012 0.025 C808+ Ih 6-MR -7.2 0.011 0.015 S=0 5-MR -4.0 0.017 C805- Ih 6-MR -20.8 0.019 0.012 S = 13/2 5-MR -5.5 0.034 J. Poater and M. Solà Chem. Commun. 2011, 47, 11647
  • 14. Open-shellsphericalaromaticity Systems symm. NICS(1)zz MCI Spin Ge122- Ih -5.5 0.049 S=0 Ge121- Ih -405.9 0.113 S = 5/2 Ge124+ Ih -69.0 0.088 S=0
  • 15. All-metal aromatic clusters • All-metal and semimetal aromatic clusters are among the most exciting molecules synthesized since the beginning of the present century. • These compounds can have not only the conventional p-(anti)aromaticity of classical organic compounds, but also - or even - and -(anti)aromaticity, thus giving rise to the so- called multifold aromaticity.
  • 16. All-metal aromatic clusters • Thetendencyofp-electrons in classicalorganicaromaticmoleculesisalwaystolocalizethedoublebond s (distortivecharacter), againstthedelocalizingforceofthe-electrons. S.C.A.H. Pierrefixe, F.M. Bickelhaupt, Chem. Eur. J. 2007, 13, 6321 • Thus, whilemany of thepropertiesattributedtoaromaticity derive fromthep-electrons, the-electrons are theonesresponsibleforthesymmetricframework of monocyclicaromaticcompounds.
  • 17. All-metal aromatic clusters • Al42-wasthefirstall-metal compoundssynthesized, containinga pair of delocalized p-electrons (orbital 1a2u) and two pairs of -electrons (orbitals 1b2g and 2a1g) that contribute to the overall aromaticity of this species. X. Li, A.E. Kuznetsov, H.F. Zhang, A.I. Boldyrev, L.S. Wang, Science 2001, 291, 859. • Thus, Al42- can be considered as a “3- fold” aromatic system ( + paromatic)
  • 18. All-metal aromatic clusters • Are the p-electrons of the Al42- cluster distortive, i.e., do they work against the regular "aromatic" structure with delocalized, equivalent bonds? Or is this propensity a characteristic of only classical aromatic organic molecules? J. Poater, F. Feixas, F.M. Bickelhaupt and M. Solà Chem. Commun. 2011, 47, 11647
  • 19. All-metal aromatic clusters • AmsterdamDensityFunctional • BP86/TZ2P, QUILD • EnergyDecompositionAnalysis ∆E : M2- (aaa) + M2- (bbb) M42- ∆E =∆Eprep + ∆Eint ∆Eint = ∆Velstat + ∆EPauli + ∆Eoi ∆Eoi = SG ∆EG ∆Eint = ∆Velstat + “total ” + “total p” J. Poater, F. Feixas, F.M. Bickelhaupt and M. Solà Chem. Commun. 2011, 47, 11647
  • 20. All-metal aromatic clusters J. Poater, F. Feixas, F.M. Bickelhaupt and M. Solà Chem. Commun. 2011, 47, 11647
  • 21. All-metal aromatic clusters 50 40 30 total  20 DEint 10 0 total p 90 92 94 96 98 100 -10 DVelstat -20 -30 •Equivalenttrendstothosefound in benzene. J. Poater, F. Feixas, F.M. Bickelhaupt and M. Solà Chem. Commun. 2011, 47, 11647
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  • 26. ACKNOWLEDGMENTS Prof. Dr. MiquelSolà(UdG) Prof. Dr. F. Matthias Bickelhaupt Dr. FerranFeixas (San Diego, USA)
  • 27. http://iqc.udg.edu 19/4/2012 Toulouse RECENT ADVANCES IN AROMATICITY 27